Replicator Dynamics and Correlated Equilibrium

Size: px
Start display at page:

Download "Replicator Dynamics and Correlated Equilibrium"

Transcription

1 Replicator Dynamics and Correlated Equilibrium Yannick Viossat To cite this version: Yannick Viossat. Replicator Dynamics and Correlated Equilibrium. CECO <hal > HAL Id: hal Submitted on 6 Feb 2008 HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d enseignement et de recherche français ou étrangers, des laboratoires publics ou privés.

2 ECOLE POLYTECHNIQUE CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE Replicator Dynamics and Correlated Equilibrium Yannick Viossat December 2004 Cahier n LABORATOIRE D'ECONOMETRIE 1rue Descartes F Paris (33) mailto:labecox@poly.polytechnique.fr

3 Replicator Dynamics and Correlated Equilibrium Yannick Viossat 1 December 2004 Cahier n Résumé: Abstract: Mots clés : Key Words : Cette note établit que dans tous les jeux 3-3 symmetriques, la dynamique des réplicateurs élimine toutes les stratégies qui ne sont utilisées dans aucun équilibre corrélé. Ce résultat s'étend à la dynamique de meilleure réponse et à toutes les dynamiques convexes monotones. La preuve repose sur des arguments de réduction duale. This note establishes that in every 3-3 symmetric game, the replicator dynamics eliminates all strategies that are never used in correlated equilibrium. This extends to the best-response dynamics and to any convex monotonic dynamics. The proof is based on dual reduction. Equilibre corrélé, dynamiques de jeux, réduction duale Correlated equilibrium, game-dynamics, dual reduction Classification JEL: C73, C72 1 Laboratoire d Econométrie, CNRS et Ecole Polytechnique

4 1 Notations, definitions and main result 1.1 Notations This note focuses on finite, two-player symmetric games. Such a game G is given by a set S = {1,..., N} of pure strategies (the same for each player) and a payoff matrix U = (U(i, j)) 1 i,j N. Here U(i, j) is the payoff of a player playing strategy i against a player playing strategy j. Since the game is symmetric, whether the player playing i is called player 1 or player 2 is unimportant. Let (S) denote the set of probabilities over S or mixed strategies: { } (S) := x R S : x i 0 i S, i S x i = 1 The payoff of a player playing the mixed strategy x against a player playing the mixed strategy y will be denoted U(x, y) := x i y j U(i, j) 1.2 Replicator Dynamics i S,j S Given some initial condition x(0) in (S), the single population replicator dynamics is given by ẋ i = x i [U(i, x) U(x, x)] where ẋ i, x i and x are taken at time t. We now define the two-population replicator dynamics. Since there are two populations, the set of pure strategies of player 1 is a priori different from the set S 2 of pure strategies of player 2; but since we only consider symmetric games, we may assimilate S 1 and S 2 and write S for both S 1 and S 2. The same remark holds for payoff matrices and we write U for both U 1 and U 2. Given an initial condition (x(0), y(0)) in (S) (S), the two-population replicator dynamics is given by: ẋ i = x i [U(i, y) U(x, y)] and ẏ i = y i [U(i, x) U(y, x)] (1) (here x (resp. y) represents the mean strategy in the population of players 1 (resp. 2)) Note that, for symmetric games and from a mathematical point of view, the single population replicator dynamics corresponds to the two-population replicator dynamics with symmetric initial conditions (that is, with x(0) = y(0)). Definition A pure strategy i in S of player 1 (resp. player 2) is eliminated by the twopopulation replicator dynamics (for some initial condition (x(0), y(0)) if x i (t) (resp. y i (t)) goes to zero as t goes to infinity. Note that, if the initial condition is symmetric (or, equivalently, in the single population framework), then the pure strategy i of player 1 is eliminated if and only if the pure strategy i of player 2 is eliminated. 1

5 1.3 Correlated equilibrium A correlated strategy is a probability distribution on the set S S of pure strategy profiles. Hence µ = (µ(s)) s S is a correlated strategy if µ(i, j) 0, (i, j) S S and (i,j) S S µ(i, j) = 1) A correlated strategy is a correlated equilibrium distribution (Aumann, 1974) if it satisfies the following incentive constraints: µ(i, j)[u(i, j) U(i, j)] 0 i S, i S j S and symmetrically µ(i, j)[u(j, i) U(j, i)] 0 i S j S, j S The Nash equilibria exactly correspond to the correlated equilibrium distributions µ that are independent; that is, such that there exists mixed strategies x and y in (S) such that: µ(i, j) = x i y j (i, j) S S. Definition The pure strategy i in S (resp. the pure strategy profile (i, j) in S S) is used in correlated equilibrium if there exists a correlated equilibrium distribution µ such that j S µ(i, j) > 0 (resp. µ(i, j) > 0). Remark 1 Due to the symmetry of the game, the existence of a correlated equilibrium distribution µ such that j S µ(i, j) > 0 is equivalent to the existence of a correlated equilibrium distribution µ such that j S µ(j, i) > 0. Thus, when we say that some pure strategy i is used (or not used) in correlated equilibrium, it is unnecessary to specify whether we see this strategy as a strategy of player 1 or as a strategy of player 2. Furthermore, due to the symmetry of the game and to the convexity of the set of correlated equilibrium distributions, a pure strategy is used in correlated equilibrium if and only if it is used in some symmetric equilibrium (i.e. in a correlated equilibrium µ such that µ(k, l) = µ(l, k) for every (k, l) in S S). Thus, we do not have to specify whether we are only interested in symmetric equilibria or not. 1.4 Main result Definition An initial condition (x(0), y(0)) of the two-population replicator dynamics is interior if for every pure strategy i in S, both x i (0) and y i (0) are positive. 2

6 Proposition Consider a 3 3 symmetric game. If the pure strategy i is not used in correlated equilibrium, then x i (t) and y i (t) both converge to 0 under the two-population replicator dynamics (1), for any interior initial condition (x(0), y(0)). As a particular case, this implies that: Corollary In every 3 3 symmetric game, every pure strategy that is not used in correlated equilibrium is eliminated by the single population replicator dynamics, for any interior initial condition (that is, for any initial condition x(0) in (S) such that x i (0) > 0 for every i in S). 2 Proof 2.1 Elements of dual reduction Let us first recall some properties of dual reduction (Myerson, 1997) on which the proof is based. Dual reduction is defined for any finite game, but, so that no new notations be needed, only two-player symmetric games are considered below. For k = 1, 2, let α k : S (S) denote a transition probability over the set of pure strategies S. The image of a pure strategy i by this mapping is a mixed strategy. Denote by α k i this mixed strategy. The vector α = (α 1, α 2 ) is a dual vector (Myerson, 1997) if for all (i, j) in S S: [U(α 1 i, j) U(i, j)] + [U(α 2 j, i) U(j, i)] 0 (2) Such a dual vector is strong (Viossat, 2004a) if the inequality (2) is strict for any strategy profile (i, j) that is not used in correlated equilibrium. It follows from (Nau & McCardle, 1990, discussion on page 432 and proposition 2) that there exists a strong dual vector and from a variant of the proof of proposition 5.26 in (Viossat, 2004a) that this strong dual vector may be assumed to be symmetric (i.e. we may assume α 1 = α 2 ). In the remaining of the paper, α denotes such a strong and symmetric dual vector. Note that if the pure strategy i is not used in correlated equilibrium, then for all j in S, the strategy profile (i, j) is not used in correlated equilibrium. Therefore (recall that α is strong): [U(α i, j) U(i, j)] + [U(α j, i) U(j, i)] > 0 (3) (Here and in the remaining of the paper, α i denotes either α 1 i or α 2 i. Since α is symmetric, i.e. α 1 = α 2 this is unambiguous.) 2.2 Properties of the replicator dynamics The only properties of the replicator dynamics that will be used in the proof are the one given below. Let i, i and p denote respectively two pure strategies and a mixed strategy of player 1. Fix an interior initial condition (x(0), y(0)). 3

7 Property 1 If there exist ɛ > 0 and a time T in R such that, for all t T, U(i, y(t)) < U(i, y(t)) ɛ, then x i (t) t + 0. Property 2 If p weakly dominates i and if there exists a pure strategy j in S 2 + = {j S, U(p, j) > U(i, j)} such that y j (t) does not go to zero as time goes to infinity, then x i (t) 0 t + Of course, the symmetric properties (i.e. on elimination of strategies of player 2) hold just as well. The fact that the replicator dynamics checks properties 1 and 2 is proved in the appendix. Property 2 imply the following better known property: Property 3 If a pure strategy is strictly dominated by a mixed strategy, then for every interior initial condition this pure strategy is eliminated by the two-population replicator dynamics. Proof. This corresponds to the special case of property 2 where S 2 + = S 2. Since a dynamics cannot eliminate all the pure strategies of a player, the result follows. 2.3 Proof of the proposition We are now ready to prove the proposition. From now on, there are only three pure strategies: S = {1, 2, 3}, and strategy 3 is not used in correlated equilibrium. The aim is to show that strategy 3 is eliminated by the replicator dynamics. By symmetry, we only need to show that x 3 (t) converges to 0. We first exploit the inequations (2) and (3). These inequations are particularly interesting in two cases: first, if j = i then (2) yields U(α i, i) U(i, i) (4) If moreover strategy i is not used in correlated equilibrium then (3) yields: In particular, U(α i, i) > U(i, i) Second, if j is α-invariant, i.e. if α j = j, then (2) yields U(α 3, 3) > U(3, 3) (5) U(α i, j) U(i, j) (6) If moreover strategy i is not used in correlated equilibrium then (3) yields: Now, distinguish the following cases: Case 1 If one of the strategies 1 and 2 is α-invariant U(α i, j) > U(i, j) (7) 4

8 Assume, for instance, that strategy 1 is α-invariant. Then, by (7), and by (6) Furthermore, taking i = 3 and j = 2 in (3) yields: U(α 3, 1) > U(3, 1) (8) U(α 2, 1) U(2, 1) (9) [U(α 3, 2) U(3, 2)] + [U(α 2, 3) U(2, 3)] > 0 Thus, at least one of the two brackets must be positive. If the first bracket is positive (subcase 1.1), i.e. if U(α 3, 2) > U(3, 2), then (5) and (8) imply that α 3 strictly dominates 3, hence x 3 (t) converges to 0 by property 3 and we are done. Otherwise (subcase 1.2), the second bracket is positive, i.e. U(α 2, 3) > U(2, 3). Together with (4) and (9) this implies that α 2 weakly dominates strategy 2, with strict inequality against strategy 3. Thus, by property 2, if x 3 (t) does not converge to 0, then y 2 (t) does. Now consider the 3 2 game obtained by eliminating the second strategy of player 2: in this reduced game, by (5) and (8), the third strategy of player 1 is strictly dominated by α 3; furthermore, since strategy 2 is weakly dominated, it follows that, in the reduced game, strategy 3 is strictly dominated by strategy 1. This implies that there exists a positive ɛ such that, once y 2 (t) is low enough, U(3, y) U(1, y) ɛ. By property 1, this implies that x 3 (t) converges to 0. Case 2 If neither strategy 1 nor strategy 2 is invariant Consider the 2 2 game G r obtained by elimination of the third strategy of both players. Since G r is a 2 2 symmetric game, it may a priori be of three kinds: Subcase 2.1 a coordination game, i.e. a game with two strict Nash equilibria and a completely mixed one Subcase 2.2 a game with a weakly or strictly dominated strategy Subcase 2.3 a trivial game, i.e. a game where the players have no influence on their own payoff. Since α is a strong dual vector and since strategy 3 is not used in correlated equilibrium, it follows from (Viossat, 2004a, proof of proposition 5.16, steps 2 and 3) that strategy 3 is transient under the Markov chain on S induced by α. This implies that the support of α 1 (resp. α 2) contains strategy 2 (resp. 1) but not strategy 3. This, in turn, implies two things: First, the game G r has no strict Nash equilibrium (indeed, if (i, j ) is a strict Nash equilibrium of G r then the inequality (2) for i = i and j = j cannot be satisfied). This rules out subcase 2.1. Second, the Markov chain on S induced by α has a unique recurrent communicating set: {1, 2}. By the basic theory of dual reduction (Myerson, 1997), this implies that the game G may be reduced, in the sense of dual reduction, into a game with a 5

9 unique strategy profile, which corresponds to a mixed strategy profile of G with support {1, 2} {1, 2}. By proposition 5.9 of (Viossat, 2004a), this implies that G has a Nash equilibrium with support {1, 2} {1, 2} and so, that G r has a completely mixed Nash equilibrium. This rules out subcase 2.2. Thus, the game G r is necessarily a trivial game. Now, only two possibilities remain: first (subcase 2.3.1), it may be that U(1, 3) = U(2, 3), so that U(1, j) = U(2, j) for all j in S. In that case, U(α i, j) = U(i, j) for every i in {1, 2} and every j in S (recall that for i in {1, 2}, α i has support in {1, 2}). Therefore, repeated applications of (3) show that strategy 3 is strictly dominated by α 3, so that x 3 (t) converges to 0. Otherwise (subcase 2.3.2), U(1, 3) U(2, 3), so that we may assume for instance U(1, 3) > U(2, 3). This implies that strategy 2 is weakly dominated by strategy 1, with strict inequality against strategy 3. Thus, if x 3 (t) does not converge to 0, then y 2 (t) does. But in the 3 2 game obtained by elimination of the second strategy of player 2, strategy 1 strictly dominates 3. Therefore, as in subcase 1.2, x 3 (t) converges to 0. 3 Extensions and comments 3.1 Other dynamics The only properties of the replicator dynamics that are used in the proof of the proposition are properties 1 to 3 of section 2.2. Thus, the proposition extends to any dynamics that satisfies these properties. This is the case in particular of the best-response dynamics of Matsui (1992) and of the convex monotonic dynamics of Hofbauer and Weibull (1996). See the appendix. 3.2 Asymmetric games When considering multi-population dynamics, there is no compelling reason to focus on symmetric games. A more general result than our proposition would consist in proving that the two-population replicator dynamics eliminates all strategies that are not played in correlated equilibrium in every 3 3 game (and not only in symmetric ones). 1. I do not know whether this is true or not. However, it may be shown that in every 2 2 game, the two-population replicator dynamics eliminates all strategy profiles that are not used in Nash equilibrium in the following sense: if the pure strategy profile (i, j) has probability zero in all Nash equilibria, then x i (t)y j (t) 0 as t + for any interior initial condition (x(0), y(0)). This implies that in every 2 2 game, the two-population replicator dynamics eliminates all strategies that are not used in Nash equilibrium. Here again, the proof relies solely on properties 1 to 3, so that this extends to the two-population best-response dynamics as well as to any two-population convex monotonic dynamics. 1 For two-player nonsymmetric games, the replicator dynamics is defined by taking x in (S 1 ), y in (S 2 ) and by replacing U by U 1 (resp. U 2 ) in the first (resp. second) equation of (1) 6

10 3.3 Nash Equilibrium Zeeman (1980, p ) studies the behaviour of the single population replicator dynamics in 3 3 symmetric games. In all the cases he considered, every strategy that is not used in symmetric Nash equilibrium is eliminated by the single population replicator dynamics, for any interior initial condition. This suggests that: Conjecture In any 3 3 symmetric game, every strategy that is not used in symmetric Nash equilibrium is eliminated by the single population replicator dynamics, for any interior initial condition. This result would be stronger than our corollary. Its proof however (if in the spirit of Zeeman (1980)) would probably be much more involved, and maybe less amenable to extensions to other dynamics and to the two-population replicator dynamics. 3.4 Higher dimensional games It seems that the result of this paper is one of the many results of game theory which holds true only in small dimensions. Indeed, in 4 4 symmetric games (and in higher dimensions), the single population replicator dynamics need not eliminate the pure strategies that are not played in correlated equilibrium. Actually, for the replicator and the best-response dynamics, as well as for every smooth payoff monotonic dynamics (for a definition of payoff monotonic dynamics, see Hofbauer and Sigmund, 1998, p. 88), there exists a 4 4 symmetric game in which, for an open set of initial conditions, all strategies that are used in correlated equilibrium are eliminated (hence, in the long run, only strategies that are NOT used in correlated equilibrium remain). See (Viossat, 2004b) for a proof and related results. A Some properties of convex monotonic dynamics and of the best-response dynamics The aim of this section is to show that every convex monotonic dynamics (in particular, the replicator dynamics), as well as the best-response dynamics, checks properties 1 to 3 of section 2.2. We actually prove a slightly more general result. Consider a two-player game with pure strategy set S k and payoff function U k for player k. Consider a dynamics of the form ẋ i = x i g i (x, y) ẏ j = y j h j (y, x) (10) where the C 1 functions g i (resp. h j ) have the property that i S 1 x i g i (x, y) = 0 (resp. j S 2 y j h j (y, x) = 0) for all (x, y) in (S 1 ) (S 2 ), so that (S 1 ) (S 2 ) and its boundary faces are invariant. The replicator dynamics corresponds to the special case g i (x, y) = U 1 (i, y) U 1 (x, y) and h j (y, x) = U 2 (j, x) U 2 (y, x). Such a dynamics (10) is convex monotonic if U 1 (p, y) > U 1 (i, y) k S 1 p k g k (x, y) > g i (x, y) 7

11 for all i in S 1, all p in (S 1 ), and all (x, y) in (S 1 ) (S 2 ), and similarly U 2 (q, x) > U 2 (j, x) k S 2 q k h k (y, x) > h j (y, x) for all j in S 2, all q in (S 2 ), and all (y, x) in (S 2 ) (S 1 ). In particular, the replicator dynamics is convex monotonic. Let i S 1 and p (S 1 ) denote respectively a pure and a mixed strategy of player 1. Fix a convex monotonic dynamics and an interior initial condition (x(0), y(0)). Proposition Assume that at least one of the following conditions holds: 1. There exist ɛ > 0 and a time T in R such that, for all t T, U 1 (i, y(t)) U 1 (p, y(t)) ɛ 2. The mixed strategy p weakly dominates i and there exists a pure strategy j in S 2 + = {j S 2, U 1 (p, j) > U 1 (i, j)} such that y j (t) does not go to zero as time goes to infinity. Then x i (t) converges to 0 as time goes to infinity. Proof. The below argument is essentially the one used by Hofbauer and Weibull (1996) to show that convex monotonic dynamics eliminate the pure strategies that are iteratively strictly dominated. Let V (x) := x i k S 1 x p k k and W (t) = V (x(t)). We have: Ẇ (t) = V (x) ( ẋ j = W (t) g i (x, y) ) p k g k (x, y) x j If condition 1 holds, then for all time t T, y(t) belongs to the compact set K ɛ = {y (S 2 ), U 1 (p, y) U 1 (i, y) + ɛ} Since for y in K ɛ, the quantity where g i (x, y) p k g k (x, y) is always positive, hence, by continuity, always greater that some positive constant α, it follows that, for t T, Ẇ αw. Therefore, t T W (t) W (T ) exp(α(t T )) This implies that x i (t), which is smaller than W (t), converges to 0. If condition 2 holds, then for all time t 0, g i (x, y) p j g j (x, y) is negative, hence W is always decreasing. Furthermore, there exists ɛ 0 and j S 2 + such that lim sup y j (t) ɛ. Since the velocity ẏ j is bounded, it follows that y(t) spends an infinite amount of time within the compact set K ɛ = {y (S 2 ), y j ɛ/2} Let τ(t) be the time spent by y in K ɛ up to time t: τ(t) = t 0 1 yj ɛ/2(y(t)) dt 8

12 (where 1 yj ɛ/2(y) is equal to 1 if y j ɛ/2 and to 0 otherwise). Since for y in K ɛ, the quantity g i (x, y) p j g j (x, y) is always positive, hence, by continuity, always greater that some positive constant α, it follows that: x i (t) W (t) W (0) exp( α τ) Since τ(t) goes to infinity, this implies that x i (t) converges to 0. Now consider the best-response dynamics (Matsui, 1992) given by: ẋ BR(y) and ẏ BR(x) where BR(y) (S 1 ) (resp. BR(x) (S 2 )) is the of set of mixed best-responses to y (resp x): BR(y) = {p (S 1 ), i S 1, U 1 (p, y) U 1 (i, y)} Fix an arbitrary initial condition (x(0), y(0)). Assuming that one of the two conditions of the above proposition holds, then, at least after some time T, the pure strategy i is not a best-response to y(t) (for the second condition, use the fact that under the best-response dynamics: if y j (t) > 0, then y j (t ) > 0 for all t t ). Therefore, x i (t) decreases exponentially to zero. Thus, the above proposition extends to the bestresponse dynamics. This implies that the best-response dynamics, as well as any convex monotonic dynamics, checks properties 1 to 3 of section 2.2. References [1] Aumann, R. (1974), Subjectivity and Correlation in Randomized Strategies, Journal of Mathematical Economics 1, [2] Hofbauer, J. and K. Sigmund (1998), Evolutionary Games and Population Dynamics, Cambridge University Press [3] Hofbauer, J and J.W. Weibull (1996), Evolutionary Selection against Dominated Strategies, Journal of Economic Theory, 71, [4] Matsui, A. (1992), Best-Response Dynamics and Socially Stable Strategies, Journal of Economic Theory, 57, [5] Myerson, R.B. (1997), Dual Reduction and Elementary Games, Games and Economic Behavior 21, [6] Nau, R.F. and K.F. McCardle (1990), Coherent Behavior in Noncooperative Games, Journal of Economic Theory 50, [7] Viossat, Y. (2004a), Properties and Applications of Dual Reduction, mimeo. [8] Viossat, Y. (2004b), Strategies Never played in Nash or Correlated Equilibrium and Dynamics, in preparation. 9

13 [9] Zeeman, E.C. (1980), Population Dynamics From Game Theory, in Global Theory of Dynamical Systems, Nitecki, A. and C. Robinson Eds, Springer, New York. 10

BERGE VAISMAN AND NASH EQUILIBRIA: TRANSFORMATION OF GAMES

BERGE VAISMAN AND NASH EQUILIBRIA: TRANSFORMATION OF GAMES BERGE VAISMAN AND NASH EQUILIBRIA: TRANSFORMATION OF GAMES Antonin Pottier, Rabia Nessah To cite this version: Antonin Pottier, Rabia Nessah. BERGE VAISMAN AND NASH EQUILIBRIA: TRANS- FORMATION OF GAMES.

More information

ECOLE POLYTECHNIQUE. Geometry, Correlated Equilibria and Zero-Sum Games. Yannick Viossat. Cahier n Décembre 2003

ECOLE POLYTECHNIQUE. Geometry, Correlated Equilibria and Zero-Sum Games. Yannick Viossat. Cahier n Décembre 2003 ECOLE POLYTECHNIQUE CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE Geometry, Correlated Equilibria and Zero-Sum Games Yannick Viossat Décembre 2003 Cahier n 2003-032 LABORATOIRE D'ECONOMETRIE 1rue Descartes

More information

ECOLE POLYTECHNIQUE. Properties of Dual Reduction. Yannick Viossat. Cahier n Décembre 2003 CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE

ECOLE POLYTECHNIQUE. Properties of Dual Reduction. Yannick Viossat. Cahier n Décembre 2003 CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE ECOLE POLYTECHNIQUE CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE Properties of Dual Reduction Yannick Viossat Décembre 2003 Cahier n 2003-031 LABORATOIRE D'ECONOMETRIE 1rue Descartes F-75005 Paris (33)

More information

A new simple recursive algorithm for finding prime numbers using Rosser s theorem

A new simple recursive algorithm for finding prime numbers using Rosser s theorem A new simple recursive algorithm for finding prime numbers using Rosser s theorem Rédoane Daoudi To cite this version: Rédoane Daoudi. A new simple recursive algorithm for finding prime numbers using Rosser

More information

A partial characterization of the core in Bertrand oligopoly TU-games with transferable technologies

A partial characterization of the core in Bertrand oligopoly TU-games with transferable technologies A partial characterization of the core in Bertrand oligopoly TU-games with transferable technologies Aymeric Lardon To cite this version: Aymeric Lardon. A partial characterization of the core in Bertrand

More information

The Core of a coalitional exchange economy

The Core of a coalitional exchange economy The Core of a coalitional exchange economy Elena L. Del Mercato To cite this version: Elena L. Del Mercato. The Core of a coalitional exchange economy. Cahiers de la Maison des Sciences Economiques 2006.47

More information

The core of voting games: a partition approach

The core of voting games: a partition approach The core of voting games: a partition approach Aymeric Lardon To cite this version: Aymeric Lardon. The core of voting games: a partition approach. International Game Theory Review, World Scientific Publishing,

More information

ECOLE POLYTECHNIQUE. Openness of the set of games with a unique correlated equilibrium. Yannick Viossat

ECOLE POLYTECHNIQUE. Openness of the set of games with a unique correlated equilibrium. Yannick Viossat ECOLE POLYTECHNIQUE CENTRE NATIONAL DE LA RECHERCHE SCIENTIFIQUE Openness of the set of games with a unique correlated equilibrium Yannick Viossat First version. November 2005. This version: June 2006

More information

A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications

A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications Alexandre Sedoglavic To cite this version: Alexandre Sedoglavic. A non-commutative algorithm for multiplying (7 7) matrices

More information

Hook lengths and shifted parts of partitions

Hook lengths and shifted parts of partitions Hook lengths and shifted parts of partitions Guo-Niu Han To cite this version: Guo-Niu Han Hook lengths and shifted parts of partitions The Ramanujan Journal, 009, 9 p HAL Id: hal-00395690

More information

On Symmetric Norm Inequalities And Hermitian Block-Matrices

On Symmetric Norm Inequalities And Hermitian Block-Matrices On Symmetric Norm Inequalities And Hermitian lock-matrices Antoine Mhanna To cite this version: Antoine Mhanna On Symmetric Norm Inequalities And Hermitian lock-matrices 015 HAL Id: hal-0131860

More information

On path partitions of the divisor graph

On path partitions of the divisor graph On path partitions of the divisor graph Paul Melotti, Eric Saias To cite this version: Paul Melotti, Eric Saias On path partitions of the divisor graph 018 HAL Id: hal-0184801 https://halarchives-ouvertesfr/hal-0184801

More information

Best linear unbiased prediction when error vector is correlated with other random vectors in the model

Best linear unbiased prediction when error vector is correlated with other random vectors in the model Best linear unbiased prediction when error vector is correlated with other random vectors in the model L.R. Schaeffer, C.R. Henderson To cite this version: L.R. Schaeffer, C.R. Henderson. Best linear unbiased

More information

Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma.

Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma. Methylation-associated PHOX2B gene silencing is a rare event in human neuroblastoma. Loïc De Pontual, Delphine Trochet, Franck Bourdeaut, Sophie Thomas, Heather Etchevers, Agnes Chompret, Véronique Minard,

More information

Characterization of Equilibrium Paths in a Two-Sector Economy with CES Production Functions and Sector-Specific Externality

Characterization of Equilibrium Paths in a Two-Sector Economy with CES Production Functions and Sector-Specific Externality Characterization of Equilibrium Paths in a Two-Sector Economy with CES Production Functions and Sector-Specific Externality Miki Matsuo, Kazuo Nishimura, Tomoya Sakagami, Alain Venditti To cite this version:

More information

A proximal approach to the inversion of ill-conditioned matrices

A proximal approach to the inversion of ill-conditioned matrices A proximal approach to the inversion of ill-conditioned matrices Pierre Maréchal, Aude Rondepierre To cite this version: Pierre Maréchal, Aude Rondepierre. A proximal approach to the inversion of ill-conditioned

More information

DYNAMICAL PROPERTIES OF MONOTONE DENDRITE MAPS

DYNAMICAL PROPERTIES OF MONOTONE DENDRITE MAPS DYNAMICAL PROPERTIES OF MONOTONE DENDRITE MAPS Issam Naghmouchi To cite this version: Issam Naghmouchi. DYNAMICAL PROPERTIES OF MONOTONE DENDRITE MAPS. 2010. HAL Id: hal-00593321 https://hal.archives-ouvertes.fr/hal-00593321v2

More information

Smart Bolometer: Toward Monolithic Bolometer with Smart Functions

Smart Bolometer: Toward Monolithic Bolometer with Smart Functions Smart Bolometer: Toward Monolithic Bolometer with Smart Functions Matthieu Denoual, Gilles Allègre, Patrick Attia, Olivier De Sagazan To cite this version: Matthieu Denoual, Gilles Allègre, Patrick Attia,

More information

Finite volume method for nonlinear transmission problems

Finite volume method for nonlinear transmission problems Finite volume method for nonlinear transmission problems Franck Boyer, Florence Hubert To cite this version: Franck Boyer, Florence Hubert. Finite volume method for nonlinear transmission problems. Proceedings

More information

Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122,

Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122, Case report on the article Water nanoelectrolysis: A simple model, Journal of Applied Physics (2017) 122, 244902 Juan Olives, Zoubida Hammadi, Roger Morin, Laurent Lapena To cite this version: Juan Olives,

More information

Completeness of the Tree System for Propositional Classical Logic

Completeness of the Tree System for Propositional Classical Logic Completeness of the Tree System for Propositional Classical Logic Shahid Rahman To cite this version: Shahid Rahman. Completeness of the Tree System for Propositional Classical Logic. Licence. France.

More information

On Symmetric Norm Inequalities And Hermitian Block-Matrices

On Symmetric Norm Inequalities And Hermitian Block-Matrices On Symmetric Norm Inequalities And Hermitian lock-matrices Antoine Mhanna To cite this version: Antoine Mhanna On Symmetric Norm Inequalities And Hermitian lock-matrices 016 HAL Id: hal-0131860

More information

Can we reduce health inequalities? An analysis of the English strategy ( )

Can we reduce health inequalities? An analysis of the English strategy ( ) Can we reduce health inequalities? An analysis of the English strategy (1997-2010) Johan P Mackenbach To cite this version: Johan P Mackenbach. Can we reduce health inequalities? An analysis of the English

More information

REVERSIBILITY AND OSCILLATIONS IN ZERO-SUM DISCOUNTED STOCHASTIC GAMES

REVERSIBILITY AND OSCILLATIONS IN ZERO-SUM DISCOUNTED STOCHASTIC GAMES REVERSIBILITY AND OSCILLATIONS IN ZERO-SUM DISCOUNTED STOCHASTIC GAMES Sylvain Sorin, Guillaume Vigeral To cite this version: Sylvain Sorin, Guillaume Vigeral. REVERSIBILITY AND OSCILLATIONS IN ZERO-SUM

More information

Vibro-acoustic simulation of a car window

Vibro-acoustic simulation of a car window Vibro-acoustic simulation of a car window Christophe Barras To cite this version: Christophe Barras. Vibro-acoustic simulation of a car window. Société Française d Acoustique. Acoustics 12, Apr 12, Nantes,

More information

Some tight polynomial-exponential lower bounds for an exponential function

Some tight polynomial-exponential lower bounds for an exponential function Some tight polynomial-exponential lower bounds for an exponential function Christophe Chesneau To cite this version: Christophe Chesneau. Some tight polynomial-exponential lower bounds for an exponential

More information

About partial probabilistic information

About partial probabilistic information About partial probabilistic information Alain Chateauneuf, Caroline Ventura To cite this version: Alain Chateauneuf, Caroline Ventura. About partial probabilistic information. Documents de travail du Centre

More information

A remark on a theorem of A. E. Ingham.

A remark on a theorem of A. E. Ingham. A remark on a theorem of A. E. Ingham. K G Bhat, K Ramachandra To cite this version: K G Bhat, K Ramachandra. A remark on a theorem of A. E. Ingham.. Hardy-Ramanujan Journal, Hardy-Ramanujan Society, 2006,

More information

On infinite permutations

On infinite permutations On infinite permutations Dmitri G. Fon-Der-Flaass, Anna E. Frid To cite this version: Dmitri G. Fon-Der-Flaass, Anna E. Frid. On infinite permutations. Stefan Felsner. 2005 European Conference on Combinatorics,

More information

ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS

ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS Abdelhafid Younsi To cite this version: Abdelhafid Younsi. ON THE UNIQUENESS IN THE 3D NAVIER-STOKES EQUATIONS. 4 pages. 212. HAL Id:

More information

Passerelle entre les arts : la sculpture sonore

Passerelle entre les arts : la sculpture sonore Passerelle entre les arts : la sculpture sonore Anaïs Rolez To cite this version: Anaïs Rolez. Passerelle entre les arts : la sculpture sonore. Article destiné à l origine à la Revue de l Institut National

More information

Full-order observers for linear systems with unknown inputs

Full-order observers for linear systems with unknown inputs Full-order observers for linear systems with unknown inputs Mohamed Darouach, Michel Zasadzinski, Shi Jie Xu To cite this version: Mohamed Darouach, Michel Zasadzinski, Shi Jie Xu. Full-order observers

More information

Easter bracelets for years

Easter bracelets for years Easter bracelets for 5700000 years Denis Roegel To cite this version: Denis Roegel. Easter bracelets for 5700000 years. [Research Report] 2014. HAL Id: hal-01009457 https://hal.inria.fr/hal-01009457

More information

Widely Linear Estimation with Complex Data

Widely Linear Estimation with Complex Data Widely Linear Estimation with Complex Data Bernard Picinbono, Pascal Chevalier To cite this version: Bernard Picinbono, Pascal Chevalier. Widely Linear Estimation with Complex Data. IEEE Transactions on

More information

On size, radius and minimum degree

On size, radius and minimum degree On size, radius and minimum degree Simon Mukwembi To cite this version: Simon Mukwembi. On size, radius and minimum degree. Discrete Mathematics and Theoretical Computer Science, DMTCS, 2014, Vol. 16 no.

More information

On the longest path in a recursively partitionable graph

On the longest path in a recursively partitionable graph On the longest path in a recursively partitionable graph Julien Bensmail To cite this version: Julien Bensmail. On the longest path in a recursively partitionable graph. 2012. HAL Id:

More information

A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications

A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications A non-commutative algorithm for multiplying (7 7) matrices using 250 multiplications Alexandre Sedoglavic To cite this version: Alexandre Sedoglavic. A non-commutative algorithm for multiplying (7 7) matrices

More information

On Poincare-Wirtinger inequalities in spaces of functions of bounded variation

On Poincare-Wirtinger inequalities in spaces of functions of bounded variation On Poincare-Wirtinger inequalities in spaces of functions of bounded variation Maïtine Bergounioux To cite this version: Maïtine Bergounioux. On Poincare-Wirtinger inequalities in spaces of functions of

More information

Coalitional Equilibria of Strategic Games

Coalitional Equilibria of Strategic Games Coalitional Equilibria of Strategic Games Rida Laraki To cite this version: Rida Laraki. Coalitional Equilibria of Strategic Games. cahier de recherche 2009-42. 2009. HAL Id: hal-00429293

More information

Cutwidth and degeneracy of graphs

Cutwidth and degeneracy of graphs Cutwidth and degeneracy of graphs Benoit Kloeckner To cite this version: Benoit Kloeckner. Cutwidth and degeneracy of graphs. IF_PREPUB. 2009. HAL Id: hal-00408210 https://hal.archives-ouvertes.fr/hal-00408210v1

More information

Solution to Sylvester equation associated to linear descriptor systems

Solution to Sylvester equation associated to linear descriptor systems Solution to Sylvester equation associated to linear descriptor systems Mohamed Darouach To cite this version: Mohamed Darouach. Solution to Sylvester equation associated to linear descriptor systems. Systems

More information

A new approach of the concept of prime number

A new approach of the concept of prime number A new approach of the concept of prime number Jamel Ghannouchi To cite this version: Jamel Ghannouchi. A new approach of the concept of prime number. 4 pages. 24. HAL Id: hal-3943 https://hal.archives-ouvertes.fr/hal-3943

More information

Unfolding the Skorohod reflection of a semimartingale

Unfolding the Skorohod reflection of a semimartingale Unfolding the Skorohod reflection of a semimartingale Vilmos Prokaj To cite this version: Vilmos Prokaj. Unfolding the Skorohod reflection of a semimartingale. Statistics and Probability Letters, Elsevier,

More information

Stickelberger s congruences for absolute norms of relative discriminants

Stickelberger s congruences for absolute norms of relative discriminants Stickelberger s congruences for absolute norms of relative discriminants Georges Gras To cite this version: Georges Gras. Stickelberger s congruences for absolute norms of relative discriminants. Journal

More information

Exact Comparison of Quadratic Irrationals

Exact Comparison of Quadratic Irrationals Exact Comparison of Quadratic Irrationals Phuc Ngo To cite this version: Phuc Ngo. Exact Comparison of Quadratic Irrationals. [Research Report] LIGM. 20. HAL Id: hal-0069762 https://hal.archives-ouvertes.fr/hal-0069762

More information

On Newton-Raphson iteration for multiplicative inverses modulo prime powers

On Newton-Raphson iteration for multiplicative inverses modulo prime powers On Newton-Raphson iteration for multiplicative inverses modulo prime powers Jean-Guillaume Dumas To cite this version: Jean-Guillaume Dumas. On Newton-Raphson iteration for multiplicative inverses modulo

More information

On the uniform Poincaré inequality

On the uniform Poincaré inequality On the uniform Poincaré inequality Abdesslam oulkhemair, Abdelkrim Chakib To cite this version: Abdesslam oulkhemair, Abdelkrim Chakib. On the uniform Poincaré inequality. Communications in Partial Differential

More information

On production costs in vertical differentiation models

On production costs in vertical differentiation models On production costs in vertical differentiation models Dorothée Brécard To cite this version: Dorothée Brécard. On production costs in vertical differentiation models. 2009. HAL Id: hal-00421171

More information

Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity

Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity Evolution of the cooperation and consequences of a decrease in plant diversity on the root symbiont diversity Marie Duhamel To cite this version: Marie Duhamel. Evolution of the cooperation and consequences

More information

Some explanations about the IWLS algorithm to fit generalized linear models

Some explanations about the IWLS algorithm to fit generalized linear models Some explanations about the IWLS algorithm to fit generalized linear models Christophe Dutang To cite this version: Christophe Dutang. Some explanations about the IWLS algorithm to fit generalized linear

More information

Linear Quadratic Zero-Sum Two-Person Differential Games

Linear Quadratic Zero-Sum Two-Person Differential Games Linear Quadratic Zero-Sum Two-Person Differential Games Pierre Bernhard To cite this version: Pierre Bernhard. Linear Quadratic Zero-Sum Two-Person Differential Games. Encyclopaedia of Systems and Control,

More information

There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31

There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31 There are infinitely many twin primes 30n+11 and 30n+13, 30n+17 and 30n+19, 30n+29 and 30n+31 Sibiri Christian Bandre To cite this version: Sibiri Christian Bandre. There are infinitely many twin primes

More information

Unbiased minimum variance estimation for systems with unknown exogenous inputs

Unbiased minimum variance estimation for systems with unknown exogenous inputs Unbiased minimum variance estimation for systems with unknown exogenous inputs Mohamed Darouach, Michel Zasadzinski To cite this version: Mohamed Darouach, Michel Zasadzinski. Unbiased minimum variance

More information

On the Griesmer bound for nonlinear codes

On the Griesmer bound for nonlinear codes On the Griesmer bound for nonlinear codes Emanuele Bellini, Alessio Meneghetti To cite this version: Emanuele Bellini, Alessio Meneghetti. On the Griesmer bound for nonlinear codes. Pascale Charpin, Nicolas

More information

The Mahler measure of trinomials of height 1

The Mahler measure of trinomials of height 1 The Mahler measure of trinomials of height 1 Valérie Flammang To cite this version: Valérie Flammang. The Mahler measure of trinomials of height 1. Journal of the Australian Mathematical Society 14 9 pp.1-4.

More information

The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle

The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle The FLRW cosmological model revisited: relation of the local time with th e local curvature and consequences on the Heisenberg uncertainty principle Nathalie Olivi-Tran, Paul M Gauthier To cite this version:

More information

New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space

New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space New estimates for the div-curl-grad operators and elliptic problems with L1-data in the half-space Chérif Amrouche, Huy Hoang Nguyen To cite this version: Chérif Amrouche, Huy Hoang Nguyen. New estimates

More information

Norm Inequalities of Positive Semi-Definite Matrices

Norm Inequalities of Positive Semi-Definite Matrices Norm Inequalities of Positive Semi-Definite Matrices Antoine Mhanna To cite this version: Antoine Mhanna Norm Inequalities of Positive Semi-Definite Matrices 15 HAL Id: hal-11844 https://halinriafr/hal-11844v1

More information

A Simple Model for Cavitation with Non-condensable Gases

A Simple Model for Cavitation with Non-condensable Gases A Simple Model for Cavitation with Non-condensable Gases Mathieu Bachmann, Siegfried Müller, Philippe Helluy, Hélène Mathis To cite this version: Mathieu Bachmann, Siegfried Müller, Philippe Helluy, Hélène

More information

A non-linear simulator written in C for orbital spacecraft rendezvous applications.

A non-linear simulator written in C for orbital spacecraft rendezvous applications. A non-linear simulator written in C for orbital spacecraft rendezvous applications. Paulo Ricardo Arantes Gilz To cite this version: Paulo Ricardo Arantes Gilz. A non-linear simulator written in C for

More information

b-chromatic number of cacti

b-chromatic number of cacti b-chromatic number of cacti Victor Campos, Claudia Linhares Sales, Frédéric Maffray, Ana Silva To cite this version: Victor Campos, Claudia Linhares Sales, Frédéric Maffray, Ana Silva. b-chromatic number

More information

Influence of product return lead-time on inventory control

Influence of product return lead-time on inventory control Influence of product return lead-time on inventory control Mohamed Hichem Zerhouni, Jean-Philippe Gayon, Yannick Frein To cite this version: Mohamed Hichem Zerhouni, Jean-Philippe Gayon, Yannick Frein.

More information

Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum

Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum Dissipative Systems Analysis and Control, Theory and Applications: Addendum/Erratum Bernard Brogliato To cite this version: Bernard Brogliato. Dissipative Systems Analysis and Control, Theory and Applications:

More information

Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan

Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan Soundness of the System of Semantic Trees for Classical Logic based on Fitting and Smullyan Shahid Rahman To cite this version: Shahid Rahman. Soundness of the System of Semantic Trees for Classical Logic

More information

Bodies of constant width in arbitrary dimension

Bodies of constant width in arbitrary dimension Bodies of constant width in arbitrary dimension Thomas Lachand-Robert, Edouard Oudet To cite this version: Thomas Lachand-Robert, Edouard Oudet. Bodies of constant width in arbitrary dimension. Mathematische

More information

Analysis of Boyer and Moore s MJRTY algorithm

Analysis of Boyer and Moore s MJRTY algorithm Analysis of Boyer and Moore s MJRTY algorithm Laurent Alonso, Edward M. Reingold To cite this version: Laurent Alonso, Edward M. Reingold. Analysis of Boyer and Moore s MJRTY algorithm. Information Processing

More information

A note on the computation of the fraction of smallest denominator in between two irreducible fractions

A note on the computation of the fraction of smallest denominator in between two irreducible fractions A note on the computation of the fraction of smallest denominator in between two irreducible fractions Isabelle Sivignon To cite this version: Isabelle Sivignon. A note on the computation of the fraction

More information

On sl3 KZ equations and W3 null-vector equations

On sl3 KZ equations and W3 null-vector equations On sl3 KZ equations and W3 null-vector equations Sylvain Ribault To cite this version: Sylvain Ribault. On sl3 KZ equations and W3 null-vector equations. Conformal Field Theory, Integrable Models, and

More information

A Simple Proof of P versus NP

A Simple Proof of P versus NP A Simple Proof of P versus NP Frank Vega To cite this version: Frank Vega. A Simple Proof of P versus NP. 2016. HAL Id: hal-01281254 https://hal.archives-ouvertes.fr/hal-01281254 Submitted

More information

Towards an active anechoic room

Towards an active anechoic room Towards an active anechoic room Dominique Habault, Philippe Herzog, Emmanuel Friot, Cédric Pinhède To cite this version: Dominique Habault, Philippe Herzog, Emmanuel Friot, Cédric Pinhède. Towards an active

More information

Dispersion relation results for VCS at JLab

Dispersion relation results for VCS at JLab Dispersion relation results for VCS at JLab G. Laveissiere To cite this version: G. Laveissiere. Dispersion relation results for VCS at JLab. Compton Scattering from Low to High Momentum Transfer, Mar

More information

The Windy Postman Problem on Series-Parallel Graphs

The Windy Postman Problem on Series-Parallel Graphs The Windy Postman Problem on Series-Parallel Graphs Francisco Javier Zaragoza Martínez To cite this version: Francisco Javier Zaragoza Martínez. The Windy Postman Problem on Series-Parallel Graphs. Stefan

More information

Numerical modification of atmospheric models to include the feedback of oceanic currents on air-sea fluxes in ocean-atmosphere coupled models

Numerical modification of atmospheric models to include the feedback of oceanic currents on air-sea fluxes in ocean-atmosphere coupled models Numerical modification of atmospheric models to include the feedback of oceanic currents on air-sea fluxes in ocean-atmosphere coupled models Florian Lemarié To cite this version: Florian Lemarié. Numerical

More information

L institution sportive : rêve et illusion

L institution sportive : rêve et illusion L institution sportive : rêve et illusion Hafsi Bedhioufi, Sida Ayachi, Imen Ben Amar To cite this version: Hafsi Bedhioufi, Sida Ayachi, Imen Ben Amar. L institution sportive : rêve et illusion. Revue

More information

On a series of Ramanujan

On a series of Ramanujan On a series of Ramanujan Olivier Oloa To cite this version: Olivier Oloa. On a series of Ramanujan. Gems in Experimental Mathematics, pp.35-3,, . HAL Id: hal-55866 https://hal.archives-ouvertes.fr/hal-55866

More information

Axiom of infinity and construction of N

Axiom of infinity and construction of N Axiom of infinity and construction of N F Portal To cite this version: F Portal. Axiom of infinity and construction of N. 2015. HAL Id: hal-01162075 https://hal.archives-ouvertes.fr/hal-01162075 Submitted

More information

A Context free language associated with interval maps

A Context free language associated with interval maps A Context free language associated with interval maps M Archana, V Kannan To cite this version: M Archana, V Kannan. A Context free language associated with interval maps. Discrete Mathematics and Theoretical

More information

RHEOLOGICAL INTERPRETATION OF RAYLEIGH DAMPING

RHEOLOGICAL INTERPRETATION OF RAYLEIGH DAMPING RHEOLOGICAL INTERPRETATION OF RAYLEIGH DAMPING Jean-François Semblat To cite this version: Jean-François Semblat. RHEOLOGICAL INTERPRETATION OF RAYLEIGH DAMPING. Journal of Sound and Vibration, Elsevier,

More information

Avalanche Polynomials of some Families of Graphs

Avalanche Polynomials of some Families of Graphs Avalanche Polynomials of some Families of Graphs Dominique Rossin, Arnaud Dartois, Robert Cori To cite this version: Dominique Rossin, Arnaud Dartois, Robert Cori. Avalanche Polynomials of some Families

More information

Tropical Graph Signal Processing

Tropical Graph Signal Processing Tropical Graph Signal Processing Vincent Gripon To cite this version: Vincent Gripon. Tropical Graph Signal Processing. 2017. HAL Id: hal-01527695 https://hal.archives-ouvertes.fr/hal-01527695v2

More information

Methods for territorial intelligence.

Methods for territorial intelligence. Methods for territorial intelligence. Serge Ormaux To cite this version: Serge Ormaux. Methods for territorial intelligence.. In International Conference of Territorial Intelligence, Sep 2006, Alba Iulia,

More information

Comment on: Sadi Carnot on Carnot s theorem.

Comment on: Sadi Carnot on Carnot s theorem. Comment on: Sadi Carnot on Carnot s theorem. Jacques Arnaud, Laurent Chusseau, Fabrice Philippe To cite this version: Jacques Arnaud, Laurent Chusseau, Fabrice Philippe. Comment on: Sadi Carnot on Carnot

More information

Some diophantine problems concerning equal sums of integers and their cubes

Some diophantine problems concerning equal sums of integers and their cubes Some diophantine problems concerning equal sums of integers and their cubes Ajai Choudhry To cite this version: Ajai Choudhry. Some diophantine problems concerning equal sums of integers and their cubes.

More information

FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM

FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM FORMAL TREATMENT OF RADIATION FIELD FLUCTUATIONS IN VACUUM Frederic Schuller, Renaud Savalle, Michael Neumann-Spallart To cite this version: Frederic Schuller, Renaud Savalle, Michael Neumann-Spallart.

More information

Thomas Lugand. To cite this version: HAL Id: tel

Thomas Lugand. To cite this version: HAL Id: tel Contribution à la Modélisation et à l Optimisation de la Machine Asynchrone Double Alimentation pour des Applications Hydrauliques de Pompage Turbinage Thomas Lugand To cite this version: Thomas Lugand.

More information

Finite element computation of leaky modes in straight and helical elastic waveguides

Finite element computation of leaky modes in straight and helical elastic waveguides Finite element computation of leaky modes in straight and helical elastic waveguides Khac-Long Nguyen, Fabien Treyssede, Christophe Hazard, Anne-Sophie Bonnet-Ben Dhia To cite this version: Khac-Long Nguyen,

More information

Influence of a Rough Thin Layer on the Potential

Influence of a Rough Thin Layer on the Potential Influence of a Rough Thin Layer on the Potential Ionel Ciuperca, Ronan Perrussel, Clair Poignard To cite this version: Ionel Ciuperca, Ronan Perrussel, Clair Poignard. Influence of a Rough Thin Layer on

More information

Quasi-periodic solutions of the 2D Euler equation

Quasi-periodic solutions of the 2D Euler equation Quasi-periodic solutions of the 2D Euler equation Nicolas Crouseilles, Erwan Faou To cite this version: Nicolas Crouseilles, Erwan Faou. Quasi-periodic solutions of the 2D Euler equation. Asymptotic Analysis,

More information

Multiple sensor fault detection in heat exchanger system

Multiple sensor fault detection in heat exchanger system Multiple sensor fault detection in heat exchanger system Abdel Aïtouche, Didier Maquin, Frédéric Busson To cite this version: Abdel Aïtouche, Didier Maquin, Frédéric Busson. Multiple sensor fault detection

More information

From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach

From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach From Unstructured 3D Point Clouds to Structured Knowledge - A Semantics Approach Christophe Cruz, Helmi Ben Hmida, Frank Boochs, Christophe Nicolle To cite this version: Christophe Cruz, Helmi Ben Hmida,

More information

Approval voting and the Poisson-Myerson environment

Approval voting and the Poisson-Myerson environment Approval voting and the Poisson-Myerson environment Matias Nunez To cite this version: Matias Nunez. Approval voting and the Poisson-Myerson environment. CECO-570. 2007. HAL Id: hal-00243049

More information

A Study of the Regular Pentagon with a Classic Geometric Approach

A Study of the Regular Pentagon with a Classic Geometric Approach A Study of the Regular Pentagon with a Classic Geometric Approach Amelia Carolina Sparavigna, Mauro Maria Baldi To cite this version: Amelia Carolina Sparavigna, Mauro Maria Baldi. A Study of the Regular

More information

The Accelerated Euclidean Algorithm

The Accelerated Euclidean Algorithm The Accelerated Euclidean Algorithm Sidi Mohamed Sedjelmaci To cite this version: Sidi Mohamed Sedjelmaci The Accelerated Euclidean Algorithm Laureano Gonzales-Vega and Thomas Recio Eds 2004, University

More information

IMPROVEMENTS OF THE VARIABLE THERMAL RESISTANCE

IMPROVEMENTS OF THE VARIABLE THERMAL RESISTANCE IMPROVEMENTS OF THE VARIABLE THERMAL RESISTANCE V. Szekely, S. Torok, E. Kollar To cite this version: V. Szekely, S. Torok, E. Kollar. IMPROVEMENTS OF THE VARIABLE THERMAL RESIS- TANCE. THERMINIC 2007,

More information

A generalized FKKM theorem and variational inequality

A generalized FKKM theorem and variational inequality A generalized FKKM theorem and variational inequality Hakim Hammami To cite this version: Hakim Hammami. A generalized FKKM theorem and variational inequality. Documents de travail du Centre d Economie

More information

Weighted Radon transforms for which the Chang approximate inversion formula is precise

Weighted Radon transforms for which the Chang approximate inversion formula is precise Weighted adon transforms for which the Chang approximate inversion formula is precise oman Novikov To cite this version: oman Novikov. Weighted adon transforms for which the Chang approximate inversion

More information

Comments on the method of harmonic balance

Comments on the method of harmonic balance Comments on the method of harmonic balance Ronald Mickens To cite this version: Ronald Mickens. Comments on the method of harmonic balance. Journal of Sound and Vibration, Elsevier, 1984, 94 (3), pp.456-460.

More information

Numerical Exploration of the Compacted Associated Stirling Numbers

Numerical Exploration of the Compacted Associated Stirling Numbers Numerical Exploration of the Compacted Associated Stirling Numbers Khaled Ben Letaïef To cite this version: Khaled Ben Letaïef. Numerical Exploration of the Compacted Associated Stirling Numbers. 2017.

More information

Nel s category theory based differential and integral Calculus, or Did Newton know category theory?

Nel s category theory based differential and integral Calculus, or Did Newton know category theory? Nel s category theory based differential and integral Calculus, or Did Newton know category theory? Elemer Elad Rosinger To cite this version: Elemer Elad Rosinger. Nel s category theory based differential

More information

Thermodynamic form of the equation of motion for perfect fluids of grade n

Thermodynamic form of the equation of motion for perfect fluids of grade n Thermodynamic form of the equation of motion for perfect fluids of grade n Henri Gouin To cite this version: Henri Gouin. Thermodynamic form of the equation of motion for perfect fluids of grade n. Comptes

More information